{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:LKOW432AQWN5J3BW2G4MTK3J3A","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"b796840f94baf9158a76736ec1207be79f8a153c939be2ae5d7694fea0f6acc7","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2025-02-05T16:30:50Z","title_canon_sha256":"169dca35917243bb14cd8781b985096f36f15c4e5ac18be5128adcddc9452204"},"schema_version":"1.0","source":{"id":"2502.03337","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2502.03337","created_at":"2026-07-05T11:44:44Z"},{"alias_kind":"arxiv_version","alias_value":"2502.03337v2","created_at":"2026-07-05T11:44:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.03337","created_at":"2026-07-05T11:44:44Z"},{"alias_kind":"pith_short_12","alias_value":"LKOW432AQWN5","created_at":"2026-07-05T11:44:44Z"},{"alias_kind":"pith_short_16","alias_value":"LKOW432AQWN5J3BW","created_at":"2026-07-05T11:44:44Z"},{"alias_kind":"pith_short_8","alias_value":"LKOW432A","created_at":"2026-07-05T11:44:44Z"}],"graph_snapshots":[{"event_id":"sha256:204e6ed5484ebeedfa331d480c6c3b8218b4c7a3608ac42df83a6cc6b10bcb0f","target":"graph","created_at":"2026-07-05T11:44:44Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2502.03337/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this letter we introduce the noncommutative geometry into the standard Einstein-Hilbert-Maxwell action via the $\\partial_t\\wedge\\partial_\\varphi$ Drinfeld twist and solve the equation of motion pertubatively in the expansion of the noncommutative parameter $a$. The equation of motion, the NC Einstein-Maxwell equation, turns out to be effectively a problem in nonlinear electrodynamics where the energy-momentum tensor $T_{\\mu\\nu}$ obtains correction terms with three Faraday tensors $F_{\\mu\\nu}$. A solution with nonzero $a^1$ terms turns out to be the Kerr-Newman black hole modified with nonze","authors_text":"Filip Po\\v{z}ar","cross_cats":["hep-th","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2025-02-05T16:30:50Z","title":"Corrections to Kerr-Newman black hole from Noncommutative Einstein-Maxwell equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.03337","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:54d62964db2643b608ebf6027254f50d900f22d2e7ab0ba661e468e2185e18c7","target":"record","created_at":"2026-07-05T11:44:44Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"b796840f94baf9158a76736ec1207be79f8a153c939be2ae5d7694fea0f6acc7","cross_cats_sorted":["hep-th","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2025-02-05T16:30:50Z","title_canon_sha256":"169dca35917243bb14cd8781b985096f36f15c4e5ac18be5128adcddc9452204"},"schema_version":"1.0","source":{"id":"2502.03337","kind":"arxiv","version":2}},"canonical_sha256":"5a9d6e6f40859bd4ec36d1b8c9ab69d805298a68eaa04cac77396955dc0df0b4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5a9d6e6f40859bd4ec36d1b8c9ab69d805298a68eaa04cac77396955dc0df0b4","first_computed_at":"2026-07-05T11:44:44.851600Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:44:44.851600Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TNYr6Gu76yOTcTNva4y6xcgIY8mOsHGgEALIYxOQVyUueMjSwVrMR0QcUebcBXHzSexV6YQQsexluxEJr6jYCg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:44:44.851978Z","signed_message":"canonical_sha256_bytes"},"source_id":"2502.03337","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:54d62964db2643b608ebf6027254f50d900f22d2e7ab0ba661e468e2185e18c7","sha256:204e6ed5484ebeedfa331d480c6c3b8218b4c7a3608ac42df83a6cc6b10bcb0f"],"state_sha256":"e4296227605b881db30155c48b477b3f6bd9273d035b16e4e6aae70f80992bf2"}